The growth exponent \(\alpha \)  depends upon several parameters [1]}, [2]}. In non-hydrodynamic environment, one expects \(\alpha =1/3\) . This is referred to as the Lifshitz-Slyozov (LS) growth law [3]}, [4]}, [5]}, [6]}, [7]}, [8]}, [9]}, [10]}, [11]} and is a result of diffusive transport of particles, via chemical potential gradient. The LS picture applies to phase separating solid mixtures and remains valid for critical as well as off-critical compositions [3]}, [4]}, for the entire growth period. In fluids, however, hydrodynamics is important. There the mechanisms and exponents are different for the above two situations that give rise, respectively, to bicontinuous and disconnected droplet morphologies [14]}, [15]}, [16]}, [17]}, [18]}, [19]}, [20]}, [21]}, [22]}, [23]}, [24]}, [25]}, [26]}, [27]}, [28]}, [29]}, [30]}, [31]}, [32]}, [33]}, [34]}, [35]}, [36]}, [37]}, [38]}. This is true for vapor-liquid as well as liquid-liquid transitions, in the former case density playing the role of composition. Below we briefly describe these in the liquid-liquid context.
